extended mhd
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2021 ◽  
Vol 28 (10) ◽  
pp. 102703
Author(s):  
J. R. Young ◽  
M. B. Adams ◽  
H. Hasson ◽  
I. West-Abdallah ◽  
M. Evans ◽  
...  
Keyword(s):  

2021 ◽  
Vol 28 (5) ◽  
pp. 052113
Author(s):  
V. I. Geyko ◽  
J. R. Angus ◽  
M. A. Dorf

2021 ◽  
Author(s):  
Matthias Hoelzl ◽  
Guido Huijsmans ◽  
Stanislas Pamela ◽  
Marina Becoulet ◽  
Eric Nardon ◽  
...  

Author(s):  
Andres Cathey ◽  
Matthias Hoelzl ◽  
Shimpei Futatani ◽  
Peter Lang ◽  
Karl Lackner ◽  
...  

2021 ◽  
Author(s):  
Shimpei Futatani ◽  
Andres Cathey ◽  
Matthias Hoelzl ◽  
Peter Lang ◽  
Guido Huijsmans ◽  
...  
Keyword(s):  

2020 ◽  
Vol 60 (12) ◽  
pp. 124007 ◽  
Author(s):  
A. Cathey ◽  
M. Hoelzl ◽  
K. Lackner ◽  
G.T.A. Huijsmans ◽  
M.G. Dunne ◽  
...  

2020 ◽  
Vol 496 (1) ◽  
pp. 223-244 ◽  
Author(s):  
Michael L Weber ◽  
Barbara Ercolano ◽  
Giovanni Picogna ◽  
Lee Hartmann ◽  
Peter J Rodenkirch

ABSTRACT High-resolution spectra of typical wind diagnostics ([O i] 6300 Å and other forbidden emission lines) can often be decomposed into multiple components: high-velocity components with blueshifts up to several 100 km s−1 are usually attributed to fast jets, while narrow (NLVC) and broad (BLVC) low-velocity components are believed to trace slower disc winds. Under the assumption that the line broadening is dominated by Keplerian rotation, several studies have found that the BLVCs should trace gas launched between 0.05 and 0.5 au and correlations between the properties of BLVCs and NLVCs have been interpreted as evidence for the emission tracing an extended magnetohydrodynamics (MHD) wind and not a photoevaporative wind. We calculated synthetic line profiles obtained from detailed photoionization calculations of an X-ray photoevaporation model and a simple MHD wind model and analysed the emission regions of different diagnostic lines and the resulting spectral profiles. The photoevaporation model reproduces most of the observed NLVCs but not the BLVCs or HVCs. The MHD model is able to reproduce all components but produces Keplerian double peaks at average inclinations that are rarely observed. The combination of MHD and photoevaporative winds could solve this problem. Our results suggest that the Gaussian decomposition does not allow for a clear distinction of flux from different wind regions and that the line broadening is often dominated by the velocity gradient in the outflow rather than by Keplerian rotation. We show that observed correlations between BLVC and NLVC do not necessarily imply a common origin in an extended MHD wind.


2019 ◽  
Vol 124 (11) ◽  
pp. 8474-8487 ◽  
Author(s):  
J. M. TenBarge ◽  
J. Ng ◽  
J. Juno ◽  
L. Wang ◽  
A. H. Hakim ◽  
...  

Fluids ◽  
2019 ◽  
Vol 4 (1) ◽  
pp. 46 ◽  
Author(s):  
Hideaki Miura

Incompressible magnetohydrodynamic (MHD) turbulence under influences of the Hall and the gyro-viscous terms was studied by means of direct numerical simulations of freely decaying, homogeneous and approximately isotropic turbulence. Numerical results were compared among MHD, Hall MHD, and extended MHD models focusing on differences of Hall and extended MHD turbulence from MHD turbulence at a fully relaxed state. Magnetic and kinetic energies, energy spectra, energy transfer, vorticity and current structures were studied. The Hall and gyro-viscous terms change the energy transfer in the equations of motions to be forward-transfer-dominant while the magnetic energy transfer remains backward-transfer-dominant. The gyro-viscosity works as a kind of hyper-diffusivity, attenuating the kinetic energy spectrum sharply at a high wave-number region. However, this term also induces high-vorticity events more frequently than MHD turbulence, making the turbulent field more intermittent. Vortices and currents were found to be transformed from sheet to tubular structures under the influences of the Hall and/or the gyro-viscous terms. These observations highlight features of fluid-dynamic aspect of turbulence in sub-ion-scales where turbulence is governed by the ion skin depth and ion Larmor radius.


2019 ◽  
Vol 26 (2) ◽  
pp. 024501 ◽  
Author(s):  
D. A. Kaltsas ◽  
G. N. Throumoulopoulos ◽  
P. J. Morrison

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